Method for measuring the content of fat/oil in a multi component system

ABSTRACT

The invention is a method for determination of the content of fat in a multicomponent system. The method applies nuclear magnetic resonance (NMR) for the determination of fat/oil in for example fillets of fish, olives, paint or ice cream.

[0001] The invention is a method for determining the amount of fat in a multicomponent system where water, sugar, protein or other components containing hydrogen maybe present. The method applies nuclear magnetic resonance (NMR) for determining the amount of fat/oil in for example fish, olives, paints, or dairy products.

[0002] There are several methods used for determining the content of fat/oil; In the Fosslet-, Soxhlet-, and Ethylacetate methods one adds solvents which extracts the fat/oil. By removing the solvent, one is left with the fat/oil which originally was found in the sample. These methods require well trained laboratory personnel and the use of toxic solvent which may damage the environment.

[0003] Another way to measure the fat/oil content is to use Near Infrared Reflectance (NIR) spectroscopy. This type of measurements require a lot of calibration work for a given system as the method is very sensitive to changes in the texture of the sample.

[0004] The purpose of the proposed method is to supply a robust method for determination of fat/oil in a generally multicomponent system. The method is fats, accurate, and it does not demand laboratory personnel who has specific knowledge with respect to the method.

[0005] This is achieved by placing the sample to be investigated in a homogeneous/static magnetic field, and being exposed to an oscillating magnetic field which in combination with a magnetic field gradient over the sample measures the nuclear magnetic moment of the protons, in a multipulsed field gradient spin-echo experiment (m- PFGSE), as one resolves the fat/oil-signal from the other components by their significant difference in mobility and/or transverse relaxation times.

[0006] Further details on the invention will be apparent in the following description of the method with reference to the figures.

[0007]FIG. 1. A multicomponent sample placed in a NMR-based spectrometer.

[0008]FIG. 2. Signal arising from the use of a multi-Pulsed magnetic Field Gradient Spin-Echo method (m-PFGSE).

[0009]FIG. 3. Result from a m-PFGSE on homogenised filet of herring, which shows the attenuation of fat/oil from a m-PFGSE due to mobility and T2*.

[0010] When placing hydrogen in an external magnetic field, the nuclear magnetic moment will align towards the direction of this field. The Hamiltonian for noninteracting nuclear magnetic spins in an external magnetic field can be written $\begin{matrix} {H = {{- \gamma}\quad \hslash \quad I\quad H_{(t)}}} & ({L1}) \end{matrix}$

[0011] where y=gyromagnetic ratio, ℏ = Planck’s   constant.

[0012] I=spin operator and H(t)=external magnetic field. The time dependency of H(t) is included in order to make (LI) valid when the system is influenced by an oscillating magnetic field ( RF-field) and magnetic field gradients (g). When the Hamiltonian, Rt), is constant and homogeneous (=Ho), the eigenvalues, the energy levels, of the hydrogen's nuclear spin may be written $\begin{matrix} {E = {{{\pm \frac{1}{2}}\quad \gamma \quad \hslash \quad H_{0}} = {{\pm \frac{1}{2}}\quad \hslash \quad \omega_{0}}}} & ({L2}) \end{matrix}$

[0013] The difference between the to energy levels is thus written $\begin{matrix} {{\Delta \quad E} = {\hslash \quad \omega_{0}}} & ({L3}) \end{matrix}$

[0014] In thermal equilibrium a difference population between upper and lower level is given by the Boltzmann factor $\begin{matrix} {\frac{n_{upper}}{n_{lower}} = ^{- \frac{\hslash \quad \omega}{kT}}} & ({L4}) \end{matrix}$

[0015] where T is absolute temperature and k1- Boltzmann's constant. The difference in population will generate a net nuclear magnetic moment which will depend on the content of hydrogen/protonL In thermal equilibrium the moment will be aligned with the external magnetic field. By imposing an oscillating magnetic field, RF-field, transverse to the external magnetic field Ho, transitions between the energy levels will occur (ref 1). The direction of the net nuclear magnetic moment will then move away from thermal equilibrium with the external field. When the RF-field is switched off, the system will z,999 characteristic relaxation times T1 (longitudinal relaxation) and T2 (transverse relaxation).

[0016] The path back to thermal equilibrium in combination with an oscillating net nuclear magnetic moment transverse to Ho, will cause changes in the magnetic flux which can be recorded with the same RF-coil which was used to excite the system. The current induced in the coil will then be proportional to the number of hydrogen in the system, and from the intensity of the signal one may quantify the content of hydrogen in the system ( FIG. 1).

[0017] One may record the mobility of the hydrogen by making use of a magnetic field gradient. This magnetic field gradient, g, imposes a position dependent frequency an the system, and with which the nuclear magnetic moment of the proton is oscillating in a plane transverse to Ho ω=γH_(o)+γgz (L5)

[0018] By using RF-pulses and magnetic field gradients in a NMR-diffusion experiment (ref 2), there is a dephasing of the net magnetic moment given by φ=γg(z₂-z₁) (L6)

[0019] (Z2-ZI) is the distance the protons has moved during the NMR- diffusion experiment. For larger values on the mobility (Z2-ZI), the induced current in the RF-coil, the NMR-signal, will decrease because of the dephasing. When assuming a Gaussian distribution of diffusivities and monoexponential attenuation of the NMR-signal due to relaxation processes, the attenuation of the NMR-signal is written $\begin{matrix} {I = {I_{0}^{- \frac{t_{1}}{T_{2}}}^{- \frac{t_{2}}{T_{1}}}^{{- \gamma^{2}}g^{2}D\quad {\int_{0}^{t}{{({\int_{0}^{t^{\prime}}{{g{(t^{''})}}{t^{''}}}})}^{2}{t^{\prime}}}}}}} & ({L7}) \end{matrix}$

[0020] t1 =duration the NMR-signal is influenced by transverse relaxation processes

[0021] t2=duration the NMR-signal is influenced by longitudinal relaxation processes

[0022] g(t”)=total magnetic field gradient, external and internal. D=diffusion coefficient T1=Characteristic longitudinal relaxation time T2=Characteristic transverse relaxation time Io=Initial intensity of the NMR-signal

[0023] There are several ways to perform a diffusion experiment by NMR. Here a so-called multi-pulsed magnetic field gradient spin echo experiment is applied ( m-PFGSE ) (see FIG. 2). FIG. 2 displays the monopolar version. With this sequence it becomes unnecessary to perform extra correction for longitudinal relaxation processes, transverse relaxation processes, and the NMR-signal will be refocused with respect to internal magnetic field gradients. In addition, the uncertainty due to eddy current field is minimised as one is using the same gradient strength throughout the experiment.

[0024] The echo-attenuation for the m-PFGSE-sequence in FIG. 2 is written $\begin{matrix} {I = {I_{0}^{{- n} \cdot {\lbrack{\frac{2\quad \tau}{T_{2}} - {\frac{2\quad \tau^{3}}{3}\gamma^{2}G_{i}^{2}D}}\rbrack}}^{{- n} \cdot {\lbrack{\gamma^{2}g^{2}D\quad {\delta^{2}{({\tau - \frac{\delta}{3}})}}}\rbrack}}}} & ({L8}) \end{matrix}$

[0025] Gi is the internal magnetic field gradient caused by changes in magnetic susceptibilities throughout the sample, g is the externally applied magnetic field gradient, 8 is the gradient pulse length, and T is the time interval between 90-degree RF-pulse and 180-degree RF- pulse.

[0026] By defining the unknown parameter $\begin{matrix} {K = {\frac{2\quad \tau}{T_{2}} + {\frac{2\quad \tau^{3}}{3}\gamma^{2}G_{i}^{2}D} + {\gamma^{2}g^{2}D\quad {\delta^{2}\left( {\tau - \frac{\delta}{3}} \right)}}}} & ({L9}) \end{matrix}$

[0027] the attenuation may be written I=I₀ e noK (LlO)

[0028] Terms including relaxation, diffusion due to internal magnetic field gradients and diffusion terms due to applied magnetic field gradients, are thus collected as one unknown, K.

[0029] To separate between NMR-signal from fat/oil and the other components, one makes use of the difference in mobility and transverse relaxation time. Fat/oil has significant different mobility from water and sugar dissolved in water. By fitting the applied field gradient pulse such that water signal and possible signal from sugar dissolved in water is suppressed at the first echo, then the m-PFGSE- experiment can be used to quantify the fat(oil) directly. Due to the very short transverse relaxation times (<I ms) of protein and solid sugar, their NMR-signal will not contribute when the first measuring point (n7O) in the m-PFGSE experiment is at 5 ms or more. The attenuation can then be written I=I_(fat) e^(−n*K) _(fat)(L11)

[0030] A weighted linear fit of the logarithm of Li 1 to the function y=−ax+c (L12)

[0031] yields a value for c where I fat=e^(c (L13))

[0032] By weighting the fit one takes into consideration that the model in (L11) is not valid at all times. When the observation time approaches 0(n ->O), the validity will increase. The first measuring points are therefore given more weight than the last ones.

[0033] Diffusion and relaxation effects in the NMR-signal is now corrected for, and the signal is meant to a measure for the content of fat(oil) on the sample.

[0034] The method is tested on homogenised salmon, herring and mackerel. Typical experimental results for homogenised herring is shown in FIG. 3. Control measurements have been performed using ethylacetate as solvent in an extraction method of fat/oil. The results from the two different methods are found in table 1. TABLE 1 NMR-results for fat content in different types of fish compared with an extraction method. Fat content by the Fat content by NMR-method/% extraction/% Wild salmon  5.5 +/− 0.1 5.3 Bred salmon 11.1 +/− 0.2 10.9 Herring 17.2 +/− 0.2 16.9 Mackerel 30.0 +/− 0.4 29.8

References

[0035] Ref. 1: NMR-Signal Reception: Virtual Photons and Coherent Spontaneous Emission, Concepts Magnetic Resonance 9: 277-297 (1997).

[0036] Ref. 2: Pulsed-Field Gradient Nuclear Magnetic Resonance as a Tool for Studying Translational Diffusion: Part I. Basic Theory, Concepts Magnetic Resonance 9: 299-336 (1997).

[0037] Ref. 3: A review ofH nuclear magnetic resonance relaxation in pathology: Are T1 and T2 diagnostics?, Medical Physics 14 (1), Jan/Feb 1987. 

1. A way to measure the content of fat or oil in a multicomponent system, characterised by a sample placed in a homogenous/static magnetic field and affected by an oscillating magnetic field (FIG. 1), which together with a magnetic field gradient measures the nuclear magnetic moment of the protons, in a multipulsed diffusion/relaxation experiment (FIG. 2), as one directly resolves the fat signal from the other components due to their differences in mobility and characteristic relaxivity.
 2. A way to measure the fat or oil content in a multicomponent system according to 1, characterised by a simultaneous correction for diffusion- and relaxation effects in the fat signal using a multipulsed diffusion/relaxation experiment (FIG. 2), by fitting the experimental result as a function of number of echoes, as the fitted signal at number of echo=0 will express the fat content. 